[0001] This invention relates to the bonding of microelectronic chips to an electrically
conducting bonding surface.
[0002] A semiconductor laser is a tiny device typically measuring only about 250 µm in width
across the mirror facets and about 400 µm in length along the optical resonator. The
active region of the laser, where recombination of holes and electrons generates stimulated
emission, is even smaller. In a typical stripe geometry, double heterostructure (DH)
laser the active region may be only 3-5 µm wide, 0.1-0.2 µm thick and 400 µm long.
As a consequence, when a typical pumping current of, say, 100 mA, is applied to the
laser, the current density in the active region may be of the order of 5000 Alcm
2. Since the lasers are commonly operated continuous wave at or near room temperature,
appreciable heating occurs. Excessive heating, of course, would damage the laser.
[0003] In order to prevent such damage, the removal of heat from the laser chip is facilitated
by bonding the chip to a suitable heat sink, which is commonly made of a high thermal
conductivity material (e.g., copper or diamond). However, the bonding operation must
be performed carefully so as to avoid inducing in the laser chip excessive strain
which, it has been found, is deleterious to laser reliability and lifetime. That is,
the common laser substrate materials, GaAs and InP, are brittle and may crack under
undue stress, e.g., 10
8 Pa (10
9 dyn/cm
2). Moreover, stress may generate defects in the active region or cause defects to
migrate to the active region.
[0004] Thus, thermo-compression and ultrasonic chip bonding, widely used techniques in the
other semiconductor fields, have been largely rejected in the semiconductor laser
art in favor of soldering in the presence of a corrosive flux. In this method, a thick
gold bonding pad is deposited on the ohmic contact on one side of the laser chip,
and a thin gold layer is formed on a Cu stud (heat sink). A thick layer of a soft,
ductile, low melting point metal (commonly indium) is evaporated onto the gold layer
on the stud and is then placed in contact with the gold bonding pad. A small weight
(e.g., 5 gm) is lowered onto the chip, and the stud temperature is raised to about
280°C in an atmosphere of forming gas in order to melt the indium and to bond the
chip to the stud. However, the indium layer tends to oxidize before the bond is completed,
and oxides in the bond area increase heat generation because of their high electrical
resistivity and poor thermal conductivity. Also, because the melting point of the
oxide is higher than that of the solder, the presence of a solid surface oxide prevents
the solder from wetting at the bonding temperature. In order to insure ease and reproducibility
in realizing these bonds, and to keep electrical conductance high, a liquid flux (e.g.,
ZnCI
27-NH
4CI-H
20) is used to dissolve the indium oxide and allow the liquid indium to flow and wet
the gold on the laser chip.
[0005] This flux soldering procedure has several drawbacks, however. First, the danger exists
of chlorine-containing residues becoming trapped within the bond. ZnCl
2, for instance, transforms into ZnO, Zn(OH)CI and HCI in the presence of small amounts
of water and thus is a potential corrosive agent in devices operated in humid ambients.
Second, the flux boils at the required bonding temperature of 260-280°C and becomes
a carrier for liquid indium droplets which, if they hit the sides of the chip, can
produce a short- circuit or cause interference with the light beam exiting the laser
facet. Third, voids 20-100 gm in size are created during bonding by bubbles of boiling
flux entrapped inside the indium. These voids can drastically affect heat removal
in the bond area because they represent barriers of practically infinite thermal resistance.
If located directly under the active region, voids can raise the junction temperature
considerably: theoretical calculations show that a 30 pm void raises the junction
temperature by 7.8°C and a 100 µm void by 47.5°C. Fourth, the bonds are frequently
incompletely wetted; i.e., the actual bond area is smaller than the gold bonding pad.
This shortcoming may be due to improper application of the flux which is applied manually
and hence is very operator dependent. Fifth, the bonds frequently contain large amounts
of Au-In intermetallic compounds (e.g., Au
4ln, Augln, Auln, and Auln
2) which can result in hard bonds. The absence of a pure indium layer after bonding
or the presence of the harder intermetallic compounds allows thermal stresses (due
to the difference in thermal expansion coefficients between the heat sink and the
laser) as well as intrinsic stresses (induced by the presence of the intermetallics)
to be transmitted to the active region of the laser.
[0006] IBM TDB Vol. 23, No. 7A December 1980 page 2990 discloses a method of bonding a microelectronic
chip to a support without using a flux. The bonding is effected in a non-oxidizing
ambient whose purpose is to prevent the formation of any oxides on the bonding material.
[0007] Forming low-stress, void-free bonds is also of interest with other microelectronic
chips, for example, LEDs which are bonded to a metallic header.
[0008] According to the present invention there is provided a method of manufacturing a
device in which a metal layer on a microelectronic chip is bonded to a metallized
support member, the method comprises providing a soft ductile bonding layer on at
least one of the metal layer and the support member, the bonding layer having a tendency
to form an oxide thereon, positioning the assembly of the support member, the chip
and the bonding layer(s) in an evacuable chamber without any liquid flux, on the bonding
layer(s), introducing gas into the chamber so that oxidation of the bonding layer
is minimized, and heating the bonding layer(s) to above the melting point thereof,
characterised in that the said gas functions as a reducing gas to reduce the oxide(s)
on the said bonding layer(s) with the consequent generation of a gaseous reduction
product, in that the pressure in the chamber is reduced to a subatmospheric pressure(s)
in order to decrease the partial pressure of the said gaseous reduction product, in
that the parts of the assembly can be brought into contact at any time, and in that
the gas, the temperature of the heating, and the reduced pressure are such that the
said gas functions as the reducing gas.
[0009] We have found that reproducible, low-strain, void-free, completely wetted, bonds
between semiconductor laser chips and their heat sinks can be realized by a fluxless
technique using a reducing gas. An embodiment method, carried out in a vacuum chamber,
entails the use of a soft, ductile metal, in the presence of the reducing gas such
as CO or substantially pure H
2, to solder a metalized heat sink to a metal layer on the chip. Preferably, the soft,
ductile metal is indium and the heat-sink is heated to a temperature in the range
of about 180-240°C when CO is used and in the range of about 220-230°C when H
2 is used. LEDs and other microelectric chips can be bonded to a bonding surface, for
example a header, in similar fashion.
[0010] The invention can be readily understood from the following, more detailed description
taken in conjunction with the accompanying drawing, in which:
Figure 1 is a schematic drawing showing a semiconductor laser chip and a heat sink
positioned in a vacuum chamber for bonding in accordance with one embodiment of our
invention;
Figure 2 is a graph showing the temperature-time profile during an illustrative bonding
operation; and
Figure 3 shows a representative distribution of stress in chips bonded at various
temperatures in embodiments of the invention.
1. Thermodynamics
[0011] Before discussing the step-by-step procedures employed in practicing our invention,
it will be instructive to consider first the thermodynamics of the reduction of the
oxide which forms on the soft, ductile metal used to effect the bond: indium sesquioxide
in the case where indium is the metal, and tin dioxide in the case where tin (usually
a Sn-Au alloy) is the metal. Based on the thermodynamics of indium sesquioxide (the
stable form at room temperature), hydrogen and carbon monoxide were chosen as the
reducing gases. The reaction with hydrogen at the bonding temperature is:

The free energy AF
T of the reduction reaction is expressed as:

where

Equation (3) shows that the equilibrium constant K is the cube of the ratio of the
partial pressures of water vapor and hydrogen, △F
0T is the free energy at 25°C and R is the ideal gas constant. In order for the reduction
reaction to proceed at temperature T, a necessary condition is:

that is,

[0012] For analytic purposes, a nominal bonding temperature of 200°C was chosen as a compromise
between two opposing tendencies: the reduction reaction becomes faster with increasing
temperature, but the bonded devices become more strained. It has been established
that the threshold for the occurrence of high strains in flux-bonded devices is 200°C,
as evidenced by the photoelastic effect. Literature values of △F
0T at 200°C average to 26.5 (±3%) kcal/mole. The value of P
H20/P
H2 calculated from Eq. (4) is 9x10-
5 (±25%). A value of this partial pressure ratio ≤9x10
-5 is therefore suitable.
[0013] The reaction with carbon monoxide is similar to the one with hydrogen,

A free energy of 11 kcal/mole was calculated from the free-energies of formation of
In
20
3, CO and C0
2 at 200°C. The calculated value of Pco
2/Pco is 2x10-
2. As before, a value of this partial pressure ratio ≤2x10
-2 is therefore suitable.
[0014] The partial pressure ratios indicate that the reduction of In
20
3 is possible provided a high enough vacuum is created in the bonding chamber and that
pure enough gases are used. More specifically, if a base vacuum of 1.33x10
-3 Pa (10
-5 Torr) is used, then Pco
2/Pco=2x10
-2 translates into a minimum P
co of about 0.05 Pa (0.5 µm) and PH
2/PH
2 translates into a minimum P
H2 of about 10 Pa (100 pm). However, the thermodynamics favor reduction with CO more
than with H
2. Similar considerations apply to the reduction of Sn0
2 where

and

at 232°C (the melting point of Sn).
2. Experimental procedure
[0015] In accordance with one embodiment of our invention, and as shown in Figure 1, an
AIGaAs DH semiconductor laser chip 10 was bonded to Au-plated Cu heat sink (or stud)
12. A gold bonding pad 14 was electroplated on the p-side electrical contact (Ti-Pt)
of the laser chip, and a layer 16 of In solder was evaporated onto the top of the
stud 12. However, it is possible (although not preferable) to form the In layer 16
on the bonding pad 14 instead of on stud 12. This procedure would entrail forming
the In layer prior to chip separation and would require care to keep In off of the
laser mirrors.
[0016] The bonding was done in a vacuum chamber 18 consisting of a bell-jar (not shown)
evacuated by a mechanical pump 19 and diffusion pump 20. The stud was held between
two spring-loaded, graphite electrodes (not shown). An electrical current applied
to these electrodes provided resistive heating of the stud 12 and In layer 16. The
surface temperature of the stud was measured with a Pt-PtRh thermocouple 22 in physical
contact with the stud surface. To eliminate systematic errors, the thermocouple was
calibrated in place in both CO and H
2 using the melting points of In on a Au-plated stud and of Sn and Pb on bare Cu studs.
[0017] After the gold pad 14 of the laser chip 10 had been positioned on the indium layer
16 on stud 12, the pressure of the vacuum chamber was reduced to about 1.33 Pa (10
-2 Torr) using the mechanical pump 19 and was then backfilled three times with the reducing
gas through entry port 21. The chamber pressure was then reduced to about 1.33x10
-3 Pa (10
-5 Torr) using the diffusion pump 20 and backfilled again. After a final pumpdown to
about 1.33x10
-3 Pa (10
-5 Torr) using the diffusion pump 20, the reducing gas was admitted to the chamber through
port 21 up to a pressure of 15-20 Pa (150-200 µm Hg). The bond was then made by applying
power to the graphite electrodes. The time-temperature cycle (Figure 2) was composed
of five parts: a first ramp (duration t
R1) from room temperature to the melting point of T
s of indium (157°C); a first plateau (duration t
s) at the melting point; a second ramp (duration t
R2) to the bonding temperature T
B; a second plateau (duration t
e) at the bonding temperature; and a fast cool-down to room temperature. In some cases
the cycle had only three parts; that is, t
s=0 and the temperature was raised from room temperature to the bonding temperature
directly. All of the devices used in the initial studies were AIGaAs DH lasers, although
this fluxless bonding technique has been used equally well with InGaAsP/InP lasers.
[0018] If a manipulator is available inside the chamber, it is possible to keep the chip
and In layer separate from one another until time t
R1+t
s+t
R2 when contact is effected between the chip and the melted solder.
3. Results with carbon monoxide
[0019] Our initial set of experiments utilized a 5 µm thick In layer, a 12 µm thick gold
pad, and a 3-part time temperature cycle with t
s=0, t
R1+t
R2=20―25 sec. and t
B=5-25 sec. The bonding temperature t
B ranged from 158°C-276°C. The strains generated in the laser chip during bonding were
imaged in an infra-red (IR) microscope using the photoelastic effect. The results
indicated that it is possible to bond chips without liquid flux in a CO ambient in
the range of temperatures 180-275°C with bonding times as low as 5 seconds. Below
180°C the bonds were nonreproducible. However, bonds with low strain, i.e. less than
about 10
7 Pa (10
8 dyn/cm
2) were achieved in the range of about 180-240°C. In comparison, stress of the order
of 10
8 Pa (10
9 dyn/cm
2) has been shown to induce ductile fracture in the epitaxial layers of a laser chip.
[0020] In another set of experiments we studied the influence of the bonding temperature
and time and of the presence or absence of a weight resting on the chip on the following
parameters: wetting, void content, bond nature (soft vs. hard) and induced stress
(measured using single crystal x-ray diffractometry in the Automatic Bragg Angle Control
(ABAC) mode, rather than using an IR microscope and the photoelastic effect. The bonding
temperature T
B varied between 167 and 230°C and the bonding time T
B between 25 and 150 sec. Different temperature profiles were examined: ramp (t
s=0; t
R1=25―60 sec.); ramp and soak at the bonding temperature (t
R1=20―35 sec., t
s=30 sec., t
R2=25 sec.); ramp and soak at temperature T
s; and slow cooling.
[0021] The devices had a 200 nm (2000 A) thick gold bonding pads 14, and studs 12 were covered
with a 1 µm thick electroplated gold layer followed by a 9 µm thick layer 16 of evaporated
indium. Bonding was achieved, as before, by bringing the stud to temperature under
a flow of CO at a pressure of 133 Pa (1 Torr) (1000 µm Hg) after several pumpdown-backfill
cycles including a final pumpdown to about 2.66x10-
3 Pa (2x10
-5 Torr). A ratio of the partial pressures

ensured the reduction of indium oxide ln
20
3 at temperatures around 200°C.
[0022] The use of a 5 gram weight resting on the laser during bonding was found to be detrimental.
In most instances, molten indium was squeezed out from under the chip resulting in
a partly or wholly intermetallic bond. Such bonds induced nonuniform stresses in the
device. In contrast, an ABAC scan taken of a chip bonded under the same conditions
of temperature and time, but without weight, exhibited a low and very uniform level
of stress along the device, viz.<0.2x10
7 Pa (<0.2x10
8 dyn/cm
2).
[0023] Practically no influence on the bonding temperature-time profile was observed within
the range studied. The only exception was a 60 sec. slow cool from 230 to 100°C which
induced nonuniform and high stresses in the device. In contrast, a single bonding
ramp (t
R1+t
R2) as short as 25 sec. yielded a satisfactory bond.
[0024] A marked influence of the temperature was observed upon the wetting characteristics.
Chips bonded at 204°C and below showed, upon debonding, that incomplete wetting of
the gold pad had occurred (island-like wetting), irrespective of the bonding time.
Chips bonded at 208°C and above exhibited complete wetting of the gold pad by the
indium.
[0025] Bonding temperatures between 208 and 223°C reproducibly kept the stress in the chips
to values lower than 0.6
X10
7 Pa (0.6x10
8 dyn/cm
2); i.e., such temperatures did not significantly affect the stress level, as compared
with that present in the chips prior to bonding. Bonding-induced stresses stated to
reach significant values at about 230°C where values as high as 1.2x10' Pa (1.2x10
8 dyn/ cm
2) were reached. The values of the stresses in weightless- and fluxless-bonded chips
are plotted versus bonding temperature in Figure 3.
[0026] Our fluxless bonding technique results in entirely void-free bonds in every instance
when complete wetting is achieved (i.e., above 204°C).
[0027] In addition, the technique is very clean in that no creeping of indium on the saw-cut
faces of the chips nor any spattering of indium on the mirror facets was ever observed.
This result is again in contrast with the flux bonding technique in which the liquid
flux acts as a carrier for indium droplets.
[0028] In summary, our fluxless bonding technique is capable of reproducibly yielding good
quality, void-free and adequately wetted bonds with a bonding temperature 75°C below
that ordinarily used for flux bonding (205 vs. 280°C). The stresses induced in the
device by this technique can reproducibly be kept below 0.6x10
7 Pa (0.6x10
8 dyn/cm2)
.
4. Results with hydrogen
[0029] These experiments were performed using chips and procedures (i.e., IR microscopy)
of the type employed in the initial experiment with CO. The bonding strains induced
in the device were high above -250°C and moderate to low below this temperature. Low-stress
bonds occurred in the range of about 220-230°C.
[0030] Three differences can be noted as compared with the results obtained in CO. First,
the lowest temperature leading to a bond was higher (220°C in H
2, 180°C in CO), which is consistent with the difference between the free-energies
of the reduction of ln
20
3 by CO and H
2. Second, all the shear tests left the bonds unaffected by a force of 150 grams indicating
that the conversion of indium to Au-In intermetallics was more complete in the presence
of H
2. That is, the interdiffusion between Au and In was faster. This conclusion is in
agreement with the observation that diffusion rates in solids are strongly dependent
on the annealing ambient. Third, the range of temperatures over which low-strain bonds
achieved was narrower: 220-230°C in H
2 but 180-240°C in CO.
[0031] As with CO, the meniscus formed by liquid indium between the gold pad and the stud
was much smaller for H
2-bonded lasers than for lasers bonded using a liquid flux.
[0032] It is to be understood that the above-described arrangements are merely illustrative
of the many possible specific embodiments which can be devised to represent application
of the invention. Numerous and varied other arrangements can be devised. In particular,
we expect similar results with Sn-alloy. solders, In-alloy solders, and with InP/InGaAsP
laser chips. Moreover, other microelectronic chips can be bonded to a metalized support
member (e.g., header or heat sink) using our technique. Finally, besides resistance
heating, other techniques, such as RF heating or radiation (laser) heating, can be
employed to effect the fluxless bond.
1. A method of manufacturing a device in which a metal layer (14) on a microelectronic
chip (10) is bonded to a metallized support member (12), the method comprises providing
a soft ductile bonding layer (16) on at least one of the metal layer and the support
member, the bonding layer(s) having a tendency to form an oxide thereon, positioning
the assembly of the support member, the chip and the bonding layer(s) in an evacuable
chamber (18) without any liquid flux on the bonding layer(s), introducing gas into
the chamber so that oxidation of the bonding layer is minimized, and heating the bonding
layer(s) to above the melting point thereof, characterised in that the said gas functions
as a reducing gas to reduce the oxide(s) on the said bonding layer(s) with the consequent
generation of a gaseous reduction product, in that the pressure in the chamber is
reduced to a subatmospheric pressure(s) in order to decrease the partial pressure
of the said gaseous reduction product, in that the parts of the assembly can be brought
into contact at any time, and in that the gas, the temperature of the heating, and
the reduced pressure are such that the said gas functions as the reducing gas.
2. The method of claim 1, characterised in that said bonding layer material comprises
a tin alloy, or indium.
3. The method of claim 2, characterised in that said gas comprises H2 or CO.
4. The method of claim 3, characterised in that the partial pressure of water vapor
P
H20 and the partial pressure of hydrogen P
H2 are related as

when using the tin alloy, and ≤9x10
-5 when using indium; or the partial pressure of carbon dioxide Pco
2 and the partial pressure of carbon monoxide P
co are related as

when using tin alloy, and ≤2x10
-2 when using indium.
5. The method of claim 4, characterised in that when using indium, the pressure of
the chamber is reduced to at least about 1.33x10-3 Pa (10-5 Torr) and either PH2 is at least about 10 Pa (100 µm Hg), or Pco is at least about 0.05 Pa (0.5 µm Hg).
6. The method of claim 10 for making a low strain bond, characterised in that the
indium bonding layer is heated in hydrogen to a temperature of about 220-230°C, or
in CO to a temperature of about 180-240°C and preferably 205-230°C.
7. The method of any one preceding claim, characterised in that the metal layer on
the chip and metallization on the support member both comprise gold.
8. The method of any one preceding claim, characterised in that the chip comprises
a semiconductor laser and the support member comprises a copper heat sink.
9. The method of any one preceding claim, characterised in that the bonding layer
is heated by applying electrical current to the heat sink.
10. The method of any one preceding claim, characterised in that the chip is a double
heterostructure comprising layers of material selected from the GaAs-AIGaAs and the
InP-InGaAsP materials systems.
1. Verfahren zum Herstellen eines Bauelementes, bei dem eine Metallschicht (14) auf
einem mikroelektronischen Chip (10) an ein metallisiertes Tragglied (12) gebondet
wird, wobei das Verfahren umfaßt
-Vorsehen einer weichen duktilen Bondschicht (16) auf wenigstens der Metallschicht
oder dem Tragglied, wobei die Schicht(en) zur Bildung eines Oxids hierauf tendiert
(tendieren),
-Positionieren der Anordnung aus Tragglied, Chip und Bondschicht(en) in einer evakuierbaren
Kammer (18) ohne jedes flüssige Flußmittel auf der (den) Bondschicht(en),
-Einführen von Gas in die Kammer, so daß eine Oxidation der Bondschicht minimiert
ist, und
-Erwärmen der Bondschicht(en) auf oberhalb deren Schmelzpunkt, dadurch gekennzeichnet,
daß
-das Gas als ein reduzierendes Gas zur Reduktion von Oxid(en) auf der (den) Bondschicht(en)
mit resultierender Erzeugung eines gasförmigen Reduktionsproduktes wirksam ist,
-der Druck der Kammer auf einen subatmosphärischen Druck oder auf subatmosphärische
Drücke reduziert wird, um den Partialdruck des gasförmigen Reduktionsproduktes zu
verringern,
-die Teile der Anordnung zu jeder Zeit in Kontakt miteinander gebracht werden können
und
-das Gas, die Erwärmungstemperatur und der reduzierte Druck so gewählt sind, daß das
Gas als das reduzierende Gas wirksam ist.
2. Verfahren nach Anspruch 1, dadurch gekennzeichnet, daß
-das Bondschichtmaterial eine Zinnlegierung oder Indium umfaßt.
3. Verfahren nach Anspruch 2, dadurch gekennzeichnet, daß
-das Gas H2 oder CO umfaßt.
4. Verfahren nach Anspruch 3, dadurch gekennzeichnet, daß
für den Partialdruck von Wasserdampf PH20 und den Partialdruck von Wasserstoff PH2 die Beziehung gilt

wenn die Zinnlegierung benutzt wird, und

wenn Indium benutzt wird, oder
-für den Partialdruck von Kohlendioxid Pco2 und den Partialdruck von Kohlenmonoxid Pco die Beziehung gilt

wenn die Zinnlegierung benutzt wird, und

wenn Indium benutzt wird.
5. Verfahren nach Anspruch 4, dadurch gekennzeichnet, daß
-bei Benutzung von Indium der Druck der Kammer auf wenigstens etwa 1,33x 10-3 Pa (10-5 Torr) reduziert wird und entweder PH2 wenigstens etwa 13,3 Pa (100 µm Hg) oder Pco wenigstens etwa 6,7x10-2 Pa (0,5 um Hg) ist.
6. Verfahren nach Anspruch 10 zum Herstellen einer Bondstelle niedriger Dehnung, dadurch
gekennzeichnet, daß die Indiumbondschicht in Wasserstoff auf eine Temperatur von etwa
220-230°C oder in CO auf eine Temperatur von etwa 180-240°C und vorzugsweise 205-230°C
erhitzt wird.
7. Verfahren nach einem der vorstehenden Ansprüche, dadurch gekennzeichnet, daß die
Metallschicht auf dem Chip und die Metallisierung auf dem Tragglied beide Gold umfassen.
8. Verfahren nach einem der vorstehenden Ansprüche, dadurch gekennzeichnet, daß das
Chip einen Halbleiterlaser umfaßt und das Tragglied eine Kupferwärmesenke umfaßt.
9. Verfahren nach einem der vorstehenden Ansprüche, dadurch gekennzeichnet, daß die
Bondschicht durch Zufuhr von elektrischem Strom zur Wärmesenke erwärmt wird.
10. Verfahren nach einem der vorstehenden Ansprüche, dadurch gekennzeichnet, daß das
Chip eine Doppelheterostruktur mit Schichten aus einem Material ist, die aus den GaAs-AIGaAs-
und den InP-lnGaAsP-Materialsystemen ausgewählt sind.
1. Un procédé de fabrication d'un dispositif dans lequel une couche de métal (14)
formée sur une puce microélectronique (10) est brasée sur un élément de support métallisé
(12), dans lequel on forme une couche de brasage tendre et ductile (16) sur l'un au
moins des éléments comprenant la couche de métal et l'élément de support, la ou les
couches de brasage ayant tendance à former un oxyde, on positionne l'ensemble de l'élément
de support, de la puce et de la couche ou des couches de brasage dans une chambre
(18) dans laquelle on peut faire le vide, sans aucun flux liquide sur la ou les couches
de brasage, on introduit un gaz dans la chambre de façon à minimiser l'oxydation de
la couche de brasage, et on chauffe la ou les couches de brasage au-dessus de leur
point de fusion, caractérisé en ce que ce gaz remplit la fonction d'un gaz réducteur
pour réduire le ou les oxydes sur la ou les couches de brasage, ce qui s'accompagne
par la génération d'un produit de réduction gazeux, en ce que la pression dans la
chambre est réduite à une ou plusieurs valeurs de pressions inférieures à la pression
atmosphérique, dans le but de diminuer la pression partielle du produit de réaction
gazeux, en ce que les éléments de l'ensemble peut être amenés en contact à n'importe
quel moment, et en ce que le gaz, la température de chauffage et la pression réduite
sont choisis de façon que ce gaz remplisse la fonction du gaz réducteur.
2. Le procédé de la revendication 1, caractérisé en ce que le matériau de la couche
de brasage consiste en un alliage d'étain ou en indium.
3. Le procédé de la revendication 2, caractérisé en ce que le gaz précité consiste
en H2 ou CO.
4. Le procédé de la revendication 3, caractérisé en ce que la pression partielle de
vapeur d'eau P
H20 et la pression partielle d'hydrogène P
H2 sont liées par la relation:

lorsqu'on utilise l'alliage d'étain, et ≤9x10
-5 lorsqu'on utilise l'indium; ou bien la pression partielle de dioxyde de carbone Pco
2 et la pression partielle de monoxyde de carbone P
co sont liées par la relation

lorsqu'on utilise un alliage d'étain, et ≤2x10
-2 lorsqu'on utilise l'indium.
5. Le procédé de la revendication 4, caractérisé en ce que lorsqu'on utilise l'indium,
on réduit la pression dans la chambre à au moins 1,33x 10-3 Pa (10-5 torr), et PH2 est au moins égale à environ 10 Pa (100 µm Hg), ou bien Pco est au moins égale à environ 0,05 Pa (0,5 pm Hg).
6. Le procédé de la revendication 10 pour réaliser une brasure à faibles contraintes,
caractérisé en ce qu'on chauffe la couche de brasage en indium dans de l'hydrogène
à une température d'environ 220-230°C, ou dans CO à une température d'environ 180-240°C,
et de préférence de 205-230°C.
7. Le procédé selon l'une quelconque des revendications précédentes, caractérisé en
ce que la couche de métal sur la puce et la métallisation sur l'élément de support
sont toutes deux en or.
8. Le procédé selon l'une quelconque des revendications précédentes, caractérisé en
ce que la puce consiste en un laser à semiconducteur et l'élément de support consiste
en un radiateur en cuivre.
9. Le procédé selon l'une quelconque des revendications précédentes, caractérisé en
ce qu'on chauffe la couche de brasage en appliquant un courant électrique au radiateur.
10. Le procédé selon l'une quelconque des revendications précédentes, caractérisé
en ce que la puce consiste en une double hétérostructure comprenant des couches de
matériaux sélectionnés parmi les systèmes de matériaux GaAs-AIGaAs et InP-InGaAsP.